This application is a continuation of application Ser. No. 07/485,806, filed Feb. 23, 1990 now abandoned, which is a continuation of application Ser. No. 07/135,489, filed Dec. 21, 1987 now abandoned, which is a continuation of application Ser. No. 06/921,727, filed Oct. 21, 1986 now abandoned.
This application is related to U.S. application Ser. No. 921,728, now abandoned filed Oct. 21, 1986 by Kiyoshi Mori, assigned to Texas Instruments, Incorporated and which is hereby incorporated into this application by this reference.
BACKGROUND OF THE INVENTIONThis invention relates to semiconductor transistors, and specifically to insulated-gate field-effect transistors, such as metal-oxide-semiconductor (MOS) transistors.
Electronic devices ranging from discrete transistors to VLSI (Very Large Scale Integration) circuits have been improved in cost and performance in many ways over the past years. One of these ways is by reducing the size of the circuit elements used. A basic circuit element is the transistor, and in the more advanced and higher density circuits, the insulated-gate field-effect transistor (IGFET). Current technology primarily uses silicon as the semiconductor and silicon-oxide as the insulator in such transistors; the resultant transistor is thus commonly called the metal-oxide-semiconductor field-effect transistor, or MOSFET. Therefore, the smaller the MOSFET that can be fabricated, the more MOSFETs that can occupy a given surface area on a silicon slice, in turn allowing the manufacture of more complex and powerful VLSI circuits at reduced cost.
Limitations in the reduction in the size of the MOSFET often exist at the dimension of the channel length of the transistor. The channel is the area between the source and drain of a MOSFET which, in digital applications, is selectively made non-conductive and conductive to effect the desired digital operation. A well defined channel is therefore essential in fabricating a functional semiconductor device. However, as the desired channel length becomes increasingly smaller, small manufacturing errors, or small particulate contaminants, can more easily cause the channel to be permanently short-circuited, rendering the transistor and the VLSI device non-functional.
In addition, as is well known in the art, the channel length controls important electrical characteristics of the device. One of these characteristics is the value of the dependence on source-to-drain current on the gate voltage, commonly called the transconductance of the device. The switching speed of the transistor increases as the transconductance of the device increases. In order to fabricate an integrated circuit having the desired electrical behavior, the transconductance of the individual transistors within the integrated circuit must be well-controlled. This requires that the channel length of the MOS transistors in such devices must be well controlled.
It is therefore desirable that MOSFETs having very small yet controllable channel lengths be incorporated into VLSI circuit designs. Heretofore, the minimum channel lengths that have been controllable have been on the order of one micron (micrometer). Current methods, primarily photolithographic in nature, have precluded substantial manufacture of smaller transistors, since it is difficult for current equipment to print patterns of smaller than one micron, with tolerances better than 20%. If channel lengths vary by 20% within a device, or from device to device, the electrical performance of the circuits will be less than desired.
The above-referenced application describes a vertical transistor having a sub-micron channel length which can be manufactured in a highly controlled manner. This transistor is made by a process which has three diffusions to create the drain, channel and source regions, and which uses a trench cut through the diffusions so that the channel of the transistor is in a vertical direction, thereby consuming a minumum of silicon surface area and also minimizing parasitic capacitance. However, while such a transistor is easily manufactured using current techniques, the operation of the transistor is not symmetric relative to source versus drain bias. It is preferable in digital logic operations that the transistor operate the same regardless of which side of the channel is biased positive (i.e., serves as the drain in n-channel MOS) relative to the other side.
The transistor disclosed in the above-referenced application is designed for small-signal applications, since the high doping densities used in its construction, as well as the short channel length, limit the diode breakdown voltage of the source-channel p-n junction, and also cause the channel region to undergo "punch-through" at a relatively low voltage. These factors thereby limit the bias voltage which can be applied to the transistor.
It is therefore an object of this invention to provide an MOS transistor structure having a short channel length less than one (micron which is fabricated by a method allowing for a high degree of channel length control, wherein the operation of the transistor is independent of which side of the channel serves as the drain region.
It is a further object of this invention to provide a vertical MOS transistor structure having the advantages of a well-controlled channel length, minimized gate-to-drain capacitance, small utilization of silicon surface area, and which is capable of high-voltage operation.
It is a further object of this invention to provide an MOS transistor having the above advantages, and which has an improved diode breakdown voltage and an improved punch-through voltage.
Other objects and advantages of the invention will become apparent to those skilled in the art, having reference to the specification and the drawings below.
BRIEF DESCRIPTION OF THE DRAWINGSFIG. 1 is a cross-sectional view of a transistor fabricated according to the invention.
FIG. 2 is a cross-sectional view of the transistor of FIG. 1, illustrating the transistor in its "on" condition.
FIGS. 3a through 3d are cross-sectional views illustrating various steps in the fabrication of the transistor of FIG. 1.
FIGS. 4a through 4c are plan views illustrating the steps illustrated in FIGS. 3b through 3d.
FIG. 5 is a cross-sectional view of the transistor of FIG. 1, further illustrating physical connection to the various regions therein.
SUMMARY OF THE INVENTIONThe invention may be incorporated in an MOS field-effect transistor in which the gate oxide is deposited in a trench, and where the channel is fabricated in a vertical direction along one side of the trench. The transistor is fabricated by diffusion of the channel region into an epitaxial layer. This diffusion can be done in a number of stages. A first implant and diffusion is for forming an isolation region between adjacent transistors; this diffusion will reach to the substrate below the epitaxial layer. A second implant and diffusion may extend from the surface of the epitaxial layer, and will serve to isolate portions of the epitaxial layer from one another, so that the source and drain regions are not shorted together. A third stage is for forming a channel region below the surface of the epitaxial layer, said channel region connected to the region formed by the second implant and diffusion. After a trench is etched which extends through the epitaxial layer into the substrate and after gate oxide is grown in the trench, a gate electrode is conformally placed adjacent to the gate oxide. This gate electrode will control the conduction in the channel from source to drain, along the side of the trench. An electrode may be connected to the channel diffusion or to the substrate, for control of the transistor threshold voltage. The use of an epitaxial region to form the source and drain regions allows symmetric operation of the transistor, as well as increased diode breakdown and punch-through voltages.
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTFIG. 1 is a cross-sectional diagram of a transistor constructed according to the preferred embodiment of the invention. This transistor is designed to have symmetry between the source and drain electrodes, to have improved diode breakdown characteristics, and also to have improved punch-through characteristics, allowing operation of the transistor at high bias voltages.
Referring to FIG. 1,substrate 20 is <100> lightly-doped p-type silicon. Drainregion 28 andsource region 32 are portions of n-typeepitaxial layer 21 which is grown onto the surface ofsubstrate 20 as the first step in fabrication of the transistor, as will be discussed below.Channel region 30 is a p-type region diffused into the n-type epitaxial layer, and is disposed betweendrain region 28 andsource region 32. At the edge ofdrain region 28 isisolation region 70, useful in isolating adjacent transistors from one another on the same semiconductor chip. Portions of n-typeepitaxial layer 21 are shown opposite from the active transistor regions to show the function ofisolation regions 70; these portions of n-typeepitaxial layer 21 may serve as source or drain regions in neighboring transistors, or merely as conductive interconnection regions.Trench 22 extends completely through the n-type epitaxial layer formingdrain region 28,gate oxide 24 is grown conformal with the walls oftrench 22, andgate electrode 26 is deposited upongate oxide 24 to form the transistor.
Electrical connection to sourceregion 32,drain region 28 andgate electrode 26 is schematically shown in FIG. 1; physical connection to these portions of the transistor may of course be made by any of the well-known methods for contacting regions within a semiconductor chip. In operation, a positive voltage is applied to drainregion 28 relative to sourceregion 32. The voltage ofgate electrode 26 is selectively controlled to control the conductivity ofchannel region 30 betweendrain region 28 andsource region 32, along the sides oftrench 22. FIG. 1 in effect shows the transistor in the condition where the voltage applied togate electrode 26 is significantly less than the voltage ofdrain region 28 plus the threshold voltage of the transistor, i.e., the channel betweendrain region 28 andsource region 32 is not conductive. It should be noted that, depending upon such factors as the charge trapped at the interface betweensubstrate 20 andgate oxide 24, and betweengate electrode 26 andgate oxide 24, as well as the dopant concentration inchannel region 30, the threshold voltage of the transistor may be less than zero; in such a case, of course, the voltage ofgate electrode 26 will be negative relative to sourceregion 32 in order to effect the condition shown in FIG. 1. In such a condition, the portion ofchannel region 30 adjacent togate oxide 24 on all sides oftrench 22 is still p-type, i.e., the majority charge carriers in said portion ofchannel region 30 are holes rather than electrons. As a result, reverse-biased p-n junctions are present betweendrain region 28 andchannel region 30, and also betweensource region 32 andchannel region 30, preventing current flow fromdrain region 28 to sourceregion 32.
Referring now to FIG. 2, the condition of the transistor of FIG. 1 is shown with the voltage applied togate electrode 26 being greater than the voltage ofsource region 32 by more than the threshold voltage of the transistor, and with a positive voltage applied to drainregion 28 relative to sourceregion 32. The positive voltage ongate electrode 26 relative to sourceregion 32 has the effect of attracting free electrons from n-type source region 32 intochannel region 30. If the voltage ofgate electrode 26 is sufficiently high, the free electrons attracted intochannel region 30 will exceed the number of holes provided by the boron dopant inchannel region 30, so that electrons, rather than holes, are the majority charge carriers in these portions ofchannel region 30. Those areas withinchannel region 30 which have been inverted from p-type to n-type are shown in FIG. 2 asinversion regions 34.Inversion regions 34 are of course adjacent togate oxide 24, i.e., at the point of the strongest electric field. The transistor threshold voltage is defined as the value of the differential voltage betweengate electrode 26 andsource region 32 at whichinversion regions 34 completely extend fromdrain region 28 to sourceregion 32. Therefore, when the gate-to-source voltage exceeds the threshold voltage as shown in FIG. 2, the p-n junctions which inhibited current flow fromdrain region 28 to sourceregion 32 are no longer present, and current can now flow fromdrain region 28 to sourceregion 32, throughinversion regions 34. The transistor action occurs since the voltage applied togate electrode 26 controls the conduction of current betweendrain region 28 andsource region 32.
As is well known in the art, if a voltage is applied to the portion of an MOS transistor into whichinversion regions 34 are to be formed, the threshold voltage can be modulated. Accordingly, a voltage applied tochannel region 30 via the electrode schematically illustrated in FIGS. 1 and 2, will affect the value of the threshold voltage of the transistor. Physical contact to channelregion 30 may either be made from the surface as suggested by FIGS. 1 and 2, or by contact tosubstrate 20. For the n-channel transistor illustrated in FIGS. 1 and 2, if a voltage is applied to channelregion 30 which is negative relative to sourceregion 32, the threshold voltage of the transistor will increase.
Referring now to FIGS. 3a through 3d, the construction of the transistor according to FIG. 1 will be explained in detail. FIG. 3a shows the initial condition ofsubstrate 20, having n-type epitaxial layer 21 grown thereupon by methods well known in the art. As an example,substrate 20 is lightly-doped p-type <100> silicon.Epitaxial layer 21 is also relatively lightly-doped, for example having an impurity concentration of 3E15 ions/cm3, with the dopant being arsenic.Epitaxial layer 21 is preferably at a thickness of 1.2 micron or less, in order to minimize parasitic gate-to-source and gate-to-drain capacitance.
FIG. 3b shows the cross-section of the transistor after the first boron (p-type) implant and diffusion creating p-type areas 73. In order to selectively dope p-type areas 73, maskinglayer 74 is placed on the surface of substrate 20 (and n-type epitaxial layer 21). Maskinglayer 74 is fabricated by methods well known in the art for providing a mask for ion implantation, such that only selected areas of a silicon substrate are implanted with the ions from the ion beam. For example, a layer of photoresist which will provide a masking film if exposed to light and developed is spun ontosubstrate 20. A photomask which is opaque in the areas which are to be implanted, and transparent in the areas which are to be shielded from the implantation, is then placed adjacent tosubstrate 20, and the surface ofsubstrate 20 is exposed to high intensity light. The photomask is removed, the photoresist developed, and the unexposed photoresist is removed fromsubstrate 20, leaving a developed photoresist layer onsubstrate 20 over those areas which are to be shielded from ion implantation. Alternatively, a photoresist which provides a masking film if developed but not exposed to light may be used with a photomask which is opaque in the areas which are to be shielded from the implantation and transparent in the areas which are to be implanted. The end result of either technique is the presence of maskinglayer 74, as shown in FIG. 3b, which will prevent energized ions from reachingsubstrate 20 in the areas it covers. Referring to FIG. 4a, maskinglayer 74 is shown in a plan view of the transistor, with the area in whichtrench 22 will be etched shown for reference.
This first boron implant, and subsequent diffusion, is intended to create the boundaries ofdrain region 28 byisolation regions 70, and also the bounds ofsource region 32 to isolate it fromdrain region 28. Accordingly, as shown in FIG. 3b, the energy of this first implant is done at a sufficiently high energy (such as 260 keV) to cause the tops of p-type regions 73 to be below the surface of n-type epitaxial layer 21, and to cause p-type regions 73 to diffuse into p-type substrate 20. A typical dose for this implant is 5E14 ions/cm2.
Referring to FIG. 3c, a cross-section of the eventual transistor is shown after a second masking operation and boron implant. This second boron implant, and subsequent diffusion, is required to complete the boundaries ofsource region 32, and to completeisolation region 70 between transistors. Referring to FIG. 3c, maskinglayer 76 is at the surface ofepitaxial layer 21 in selected areas, by way of photolithography as before. FIG. 4b shows the relationship of maskinglayer 76 to maskinglayer 74; it should be noted that maskinglayer 76 leaves substantially same area exposed as maskinglayer 74 for isolation around the transistor. The region whichmasking layer 76 leaves exposed which is within maskinglayer 74 is necessary to isolatesource region 32 fromdrain region 28, as will be shown below. P-type regions 78 are formed by the second implant and subsequent diffusion, p-type regions 78 overlapping into p-type regions 73 from the first boron implant and diffusion. At the right of FIG. 3c, for example, p-type region 78 overlaps into p-type region 73 (from FIG. 3b) to formisolation region 70. This second boron implant can be done with a relatively low energy levels, such as 50 keV, and with doses in the neighborhood of 8E14 ions/cm2.
FIG. 3d illustrates the cross-section of the transistor after a third boron p-type implant and diffusion. This third implant and diffusion is required to form the portion ofchannel region 30 extending under the portion of n-type epitaxial layer 21 which will formsource region 32. As before, maskinglayer 80 is formed on selected areas of the surface ofepitaxial layer 21 by means of well-known photolithographic techniques. Referring to FIG. 4c, maskinglayer 80 is illustrated by illustration of exposed region 80'; exposed region 80' (the portion of the silicon which is not covered by masking layer 80) is used in FIG. 4c for clarity. The area shown in FIG. 4c by exposed region 80' will be implanted by boron ions in this third implant step. The third boron implant is done at a relatively high energy, such as 200 keV, in order to concentrate the boron dopant at a depth below the surface of n-type epitaxial layer 21. As shown in FIG. 3d, p-type region 82 is so formed by the third boron implant in the area not masked by maskinglayer 80. For example a 200 keV average carrier concentration inchannel region 30 of 4E16 holes/cm3. In FIG. 3d, the combination of the three boron implants is shown aschannel region 30, the portion of n-type epitaxial layer 21 above p-type region 30 is shown assource region 32, and the portion of n-type epitaxial layer 21 below p-type region 30 is shown asdrain region 28.
Completion of the construction of the transistor requires etching oftrench 22, growth or deposition ofgate oxide 22, deposition ofgate electrode 26, and electrical interconnection ofdrain region 28,source region 30,gate electrode 26, and possibly channelregion 30. The fabrication techniques for completing the transistor are quite varied in the art, many such arrangements being useful in connection with the transistor described herein. A simple example of such an arrangement is illustrated in FIG. 5.
Referring to FIG. 5, after the implant and diffusion steps described in detail above which formupper source region 32,lower drain region 28 Midelle andchannel region 30,trench 22 is etched into the device.Trench 22 may be etched in the desired location, using techniques well known in the art, to extend through epitaxial layer 21 (i.e., through drain region 28) intosubstrate 20. Similarly as discussed in said application Ser. No. 921,728, parasitic gate-to-drain capacitance is minimized bytrench 22 fully extending throughdrain region 28. Either before or after etching oftrench 22,isolation oxide layer 60 may be either grown or deposited at selected locations on the top face oflayer 21, also using techniques well known in the art.Isolation oxide layer 60 isolates the diffused regions from potential applied togate electrode 26 and other interconnecting lines, because without sufficient oxide or other dielectric material under any extension ofgate electrode 26 on the top face oflayer 21, the potential applied togate electrode 26 may be sufficient to turn on parasitic transistors formed at the top face oflayer 21 by p-type regions disposed between two n-type regions in other areas of the device. After the placement ofisolation oxide 60,gate oxide 24 is either grown or deposited to conformally coat the walls oftrench 22,gate oxide 24 having a thickness of approximately 100 angstroms. A grown oxide is preferable forgate oxide 24 from an oxide quality standpoint; it should be noted thatgate oxide 24 will also grow at the silicon interface underisolation oxide 60. Subsequent to the growth ofgate oxide 24, a layer of polysilicon is deposited upon the top face, patterned and etched as desired to formgate electrode 26 and other conductive interconnections onsubstrate 20.Multilevel oxide layer 62 is then deposited to insulategate electrode 26 from subsequent metallization interconnection lines.
Electrical connection to the active regions of the device are next made by currently available techniques in the art. In order to make contact to drainregion 28 andsource region 32, contact vias are etched throughmultilevel oxide layer 62,isolation oxide layer 60 andgate oxide 24; diffusion of additional arsenic or phosphorous is then performed intosource region 32 or drainregion 28, as indicated bydiffusion areas 64. N-type diffusion areas 64 more heavilydope source region 28 and drainregion 32 to improve the ohmic contact between the subsequent metallization and said n-type regions. In order to make contact to sourceregion 32 and drainregion 28, metallization layer 68 (consisting of a metal such as aluminum) is deposited, patterned and etched to contact to sourceregion 32 and drainregion 28. Contact (not shown) will similarly be made togate electrode 26 by metallization layer 68 throughmultilevel oxide 62. A protective passivation overcoat (not shown) may be deposited over the whole of the structure of FIG. 5 for protection from mechanical scratches, contaminants, and moisture. It should be noted thatchannel region 30 may also have its own contact at the surface, or may use a connection to the bottom side ofsubstrate 20 for the application of a bias voltage. Other variations to the transistor structure shown in FIG. 5 obvious to those skilled in the art may be utilized for specific purposes or in specific manufacturing processes without departing from the spirit of the invention, including but not limited to double-level polysilicon layers, double-level metallization, and use of an epitaxial substrate.
The transistor of FIG. 5, constructed as described above, has a channel length of 0.4 micron, an average carrier concentration inchannel region 30 of 4E16 holes/cm3 and an average carrier concentration insource region 32 and drainregion 28 of 3E15 electrons/cm3.Source region 32 and drainregion 28 are each approximately 0.4 micron thick.
Copending application Ser. No. 921,728, incorporated by reference hereinabove, discloses a vertical MOS transistor where the drain, channel and source regions are fabricated by a triple diffusion process, i.e., the drain (n-type) diffusion is followed by a channel (p-type) diffusion, which is followed by a source (n-type) diffusion. This transistor is similar in structure to the transistor of FIG. 1, but certain features limit its use in many applications. First of all, both the channel region and source region of the triple-diffused transistor are heavily doped, since the p-type channel diffusion must overcome the n-type drain diffusion, and since the n-type source diffusion must overcome the p-type channel diffusion. As a result, the triple-diffused transistor has operating characteristics when the source is biased positive relative to the drain which are different from those when the drain is biased positive to the source. It is however preferable for transistors in a logic circuit to operate symmetrically, with the operation of the transistor independent of the bias of source versus drain.
The construction of the transistor of FIG. 5, however, provides for symmetric operation of the transistor of FIG. 1 since the carrier concentration ofdrain region 28 andsource region 28 are substantially equal to one another, as they are each formed out ofepitaxial layer 21, grown onsubstrate 20 prior to the fabrication ofchannel region 30 andtrench 22. In the example discussed herein, the carrier concentration insource region 32 and drainregion 28 is approximately 3E15 electrons/cm3.
The relatively high carrier concentrations in the source and channel regions of the triple-diffused transistor contribute to other limitations of the device. First, as is well known in the art, the avalanche breakdown voltage of a p-n junction increases as the impurity concentration on the lightly-doped side of the junction decreases. Since the lightly doped side (the channel side) of the source-channel p-n junction of the triple diffused transistor is itself rather heavily doped, this junction will have a relatively low diode breakdown voltage, limiting use of the triple-diffused transistor in power or other high-voltage applications. Secondly, sincechannel region 30 of the transistor of FIG. 1 (and the triple-diffused vertical transistor) is less than a micron, punch-through ofchannel region 30 can occur in the event bothsource region 32 and drainregion 28 are at a higher voltage thanchannel region 30, causing the depletion regions from the two reverse biased p-n junctions to come in contact with each other.
The transistor of FIG. 5 constructed according to the invention, provides for diode breakdown voltages of over 100 V, since the lightly doped side of the junction betweenchannel region 30 andsource region 32 is 3E15 electrons/cm3. Relative to the punch-through ofchannel region 30, sincesource region 32 and drainregion 28 are lightly doped relative to channelregion 30, the bulk of the depletion regions in the reverse biased condition will extend into the n-type regions, rather than intochannel region 30. As a result, even thoughchannel region 30 is only 0.4 microns long, punch-through will not occur withsource region 32 and drainregion 28 at a voltage 20 V higher than the voltage ofchannel region 30. Such operating characteristics allow the transistor of FIG. 5 to be useful in logic circuits requiring symmetric source-drain operation, and in power circuits where the relative voltages can be in the 20 V range.
Although the invention has been described in detail herein with reference its preferred embodiment, it is to be understood that this description is by way of example only, and is not to be construed in a limiting sense. It is to be further understood that numerous changes in the details of the embodiment of the invention, and additional embodiments of the invention, will be apparent to, and may be made by, persons of ordinary skill in the art without departing from the scope and spirit of the invention.